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Trajectories from the repository to the seabed in the small scale model for a realization and Us corresponding upscaled realization.

Trajectories generated from the sine circle map, Eq. for

Trajectories in 11 15 s of latex particles diam.

Trajectories in a 100 m cube

Trajectories in a structured well .

Trajectories in an unstructured well .

Trajectories in the -plane

Trajectories in the bromate chlorite-iodide system of complex oscillations in a space whose axes are absorbance at 460 nm Cg

Trajectories in the Bykov model.

Trajectories in the Henon-Heiles potential for the initial condition

Trajectories in the metastable region for different values of the interfacial tension

Trajectories in the metastable region predicted by using a nucleation growth model for several values of the interfacial tension r0.

Trajectories in the phase plane for Monod kinetics with the six classes of transient behavior from

Trajectories in the presence of external interferences. The lack of intervening controls in the presence of a strong wind results in an nndesired trajectory that does not reach the intended target.

Trajectories in the scattering by a Lennard-Jones potential

Trajectories in the X versus T

Trajectories jorl2 atoms in the MD simulations ojmotion in van der Wools clusters at two different temperatures, with average energies significantly below .

Trajectories observed during Ab initio direct dynamics trajectory caicuiations.

Trajectories of

Trajectories of -Jvinctive Processes

Trajectories of 0i of the 42nd and the 58th phenyl rings at 127 C

Trajectories of a 15 rm fluorescent particle and 4.85 and 25 irm non-fluorescent particles. They are obtained by superposing a series of consecutive images of the moving particles. The 15 pm particle shows longer streak because of its increased velocity in the dispensing branch D. Under the same exposure time, faster motion causes longer streaks.

Trajectories of a Brownian motion W.

Trajectories of a particle which interacts with a center of force via a Lennard-Jones potential for various reduced impact parameters b bla. As b increases from 0, the path changes from a head-on to a glancing collision. Plots are for different reduced collision energies, T pclJle

Trajectories of a PN receiving an inhibitory synaptic input at t 0 for different rntial states 9.



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